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利用LAMMPS建立8×8×8原子箱,采取EAM模拟大量铁原子体系。先对体系升温,让体系充分均匀,然后对体系进行不同冷却速度下的降温。经过分子动力学模拟得到能量温度曲线、径向分布函数(RDF)和体系结构。结果表明:冷却速度低于1.8×1010K/s时,结晶相变点和熔点基本重合;冷却速度超过1012K/s时,生成物为非晶;铁熔体的过冷度可达到700 K;冷却速度在1011K/s附近时,能够生成体心立方的Fe单晶。
Abstract:Establishes 8×8×8 atomic box with LAMMPS,adopts EAM(embedded atom model)potential,to simulate large number iron atoms system. At first,heats up the system,then cool downthe system under different cooling rate. Through molecular dynamics simulation,obtains energy-tem-perature curve,radial distribution function(RDF)and architecture. The results show that the crystal-lization temperature point is basically in coincident with the melting point when the cooling rate islower than 1.8×1010K/s;the product is amorphous when the cooling rate is higher than 1012K/s;thedegree of supercooling can reach 700 K;Fe single crystal can be prepared at cooling rate around1011K/s.
[1]ZHOU Y H,NIE C,TIAN H Y,et al.Investigation on the synthesis mechanism ofβ-FeSi2prepared by pulsed laser deposition[J].Wuhan University Journal of Natural Sciences,2012,17(1):61-66.
[2]陈景榕,李承基.金属与合金中的固态相变[M].北京:冶金工业出版社,1997:13-16.
[3]邵琛玮,王振华,李艳男,等.AuCu249合金团簇热稳定性的原子尺度计算研究[J].物理学报,2011,60(8):083602-083610.
[4]王丽,边秀房,李辉.金属Cu熔化结晶过程的分子动力学模拟[J].化学物理学报,2000,13(5):544-550.
[5]陈光,傅恒志.非平衡凝固新型金属材料[M].北京:科学出版社,2004:1-19.
[6]MOULSON A J,HERBERT J M.Electroceramics:materials,properties,applications[M].2nd ed.Hoboken,NJ:John Wiley&Sons,2003:122-125.
基本信息:
DOI:10.16389/j.cnki.cn42-1737/n.2014.03.003
中图分类号:O561
引用信息:
[1]周幼华,李雯慧,陶蕾等.铁熔体快速冷却过程的分子动力学模拟[J].江汉大学学报(自然科学版),2014,42(03):37-40.DOI:10.16389/j.cnki.cn42-1737/n.2014.03.003.
基金信息:
国家自然科学基金资助项目(61240056)